When a high-voltage electrical discharge is passed through a sample of hydrogen gas at low pressure, the result is individual isolated hydrogen atoms that emit a red light.
The color of the light emitted by the hydrogen atoms does not depend greatly on the temperature of the gas in the tube.
When the emitted light is passed through a prism, only a few narrow lines of particular wavelengths, called a line spectrum, are observed rather than a continuous range of wavelengths.
The light emitted by hydrogen is red because, of its four characteristic lines, the most intense line in its spectrum is in the red portion of the visible spectrum.
Johann Balmer showed that the frequencies of the lines observed in the visible region of the hydrogen line spectrum fit a simple equation where n = 3, 4, 5, 6. These lines are known as the Balmer series.
Johannes Rydberg restated and expanded Balmer's result in the Rydberg equation where n1 and n2 are positive integers, nh>nl, and Rh (the Rydberg constant) has a value of 1.09737 x 10^7 m-1.
Rydberg's equation described the wavelengths of the visible lines in the emission spectrum of hydrogen and predicted the wavelengths of other series of lines that would be observed.
Niels Bohr proposed a theoretical model for the hydrogen atom that explained its emission spectrum.
Bohr's model assumption: the electron moves around the nucleus in circular orbits that can have only a certain allowed radii and that the electron could occupy only certain regions of space.
As n decreases, the energy holding the electron and the nucleus together becomes increasingly negative; the radius of the orbit shrinks and more energy is needed to ionize the atom.
The orbit with n = 1 is the lowest lying and most tightly bound.
Because a hydrogen atom with its one electron in this orbit has the lowest possible energy, this is the ground state.
The ground state is the most stable arrangement of electrons for an element or compound.
A hydrogen atom with an electron in an orbit with n > 1 is in an excited state, any arrangement of electrons that is higher in energy that the ground state.
When an atom in an excited state undergoes a transition to the ground state (decay), it loses energy by emitting a photon whose energy corresponds to the difference in energy between the two states.
Electrons can occupy only certain regions of space, called orbits.
Orbits closer to the nucleus are lower in energy.
Electrons can move from one orbit to another by absorbing or emitting energy, giving rise to characteristic spectra.
If white light is passed through a sample of hydrogen, hydrogen atoms absorb energy as an electron is excited to higher energy levels.
If the light that emerges is passed through a prism, it forms a continuous spectrum with black lines corresponding to transitions.
Any given element has a characteristic emission spectrum and a characteristic absorption spectrum, which are complementary images.
Emission and absorption spectra form the basis of spectroscopy, which uses spectra to provide information about the structure and composition of a substance or object.
An electrical discharge excites neutral atoms to a higher energy state and light is emitted when the atoms decay to the ground state.